Heat balance for the high-temperature component of a solar flare

✍ Scribed by André Duijveman

• Publisher: Springer
• Year: 1983
• Tongue: English
• Weight: 740 KB
• Volume: 84
• Category: Article
• ISSN: 0038-0938
• DOI: 10.1007/bf00157456

✦ Synopsis

Shortly after the occurrence of the impulsive spikes of the two-ribbon flare of May 21, 1980, a temperature analysis of the X-ray emitting flare plasma showed the presence of a low-temperature component [n = 15 • 101~ cm-3; T = 20 x 106 K] and a high-temperature component [n = 2 • 101~ cm 3; T = 40 • 106 K].

The mean free path of an electron in the hot component is comparable to the size of the source ( ~ 104 km), Heat losses from the hot source can therefore not be described with classical formulae.

Theoretical arguments show that most likely the electron to ion temperature ratio Te/T i in the hot plasma is close to unity. This implies the presence of a hot ion component (T, ~ 40 • 106 K) as well. Under these conditions (T e ~ T t) heat flux limitation by electrostatic turbulence is ineffective. However, reduction of the heat flux is still possible due to the breakdown of classical theory. It is demonstrated that only non-classical current dissipation processes can sustain a hot source against cooling by a saturated heat flux.

Investigation of the collisionality as a function of position along a magnetic loop shows that the breakdown of classical theory should be expected to occur first near the base of the loop.

We conclude that the newly discovered hot source is important for the energy budget of the flare, even if the heat losses are considerably reduced. It is estimated that for the May 21, 1980 flare a total of about 1031 ergs were necessary to maintain the hot source against heat losses over the time period that it was observed (~ 10 rain).